Navigating the Cosmic Questions: Gravity Assists, Neutrinos, and Time Dilation Explained
Space Nuts: Astronomy Insights & Cosmic DiscoveriesSeptember 21, 2026
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00:30:5228.32 MB

Navigating the Cosmic Questions: Gravity Assists, Neutrinos, and Time Dilation Explained

Space Nuts: Q&A on BepiColombo, Neutrinos, and Time Dilation
In this Q&A edition of Space Nuts, hosts Andrew Dunkley and Professor Fred Watson dive into a series of intriguing listener questions that span topics from the nuances of orbital velocity to the enigmatic world of neutrinos and the complexities of time dilation. Join them as they unravel these cosmic queries with their signature blend of insight and humour.
Key topics
- Larry from Nebraska asks about the BepiColombo mission and the relationship between gravitational assists and orbital velocity, prompting a discussion on how spacecraft navigate the solar system.
- Eduardo explores the nature of neutrinos, questioning whether they are affected by gravity and whether they can be trapped by black holes.
- Shumo presents a thought-provoking idea about using high-energy gamma rays or neutrinos as interstellar beacons, leading to a discussion on the potential for advanced civilisations to communicate through unconventional means.
- Colin from Adelaide raises questions about time dilation effects as depicted in the science fiction movie "Project Hail Mary," specifically the implications of travelling close to the speed of light and the resulting age differences upon return to Earth.
Timestamps
00:00 - Introduction to the Q&A format and listener interactions
01:20 - Larry's question about BepiColombo and gravitational assists
10:30 - Eduardo's inquiry on neutrinos and black holes
18:45 - Shumo's question about interstellar beacons using gamma rays or neutrinos
26:00 - Colin's confusion about time dilation in "Project Hail Mary"
32:15 - Discussion on the implications of time dilation and relativity

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00:00:00 --> 00:00:00 Professor Fred Watson: Hi there.

00:00:00 --> 00:00:02 Andrew Dunkley: Thanks for joining us. This is Space Nuts, a

00:00:02 --> 00:00:04 Q and A edition, and we've got a bunch of

00:00:04 --> 00:00:07 questions to get through. Uh, Larry wants to

00:00:07 --> 00:00:10 know about orbital velocity and his question

00:00:10 --> 00:00:12 is quite timely because he brings up the

00:00:12 --> 00:00:15 BepiColombo mission. And we have an update

00:00:15 --> 00:00:18 on that. Uh, Eduardo is

00:00:18 --> 00:00:20 asking us about neutrinos. In fact, these

00:00:20 --> 00:00:23 last three questions dovetail into each

00:00:23 --> 00:00:25 other. So Eduardo about neutrinos. Uh,

00:00:25 --> 00:00:28 Shumo is asking about interstellar beacons

00:00:28 --> 00:00:30 that might be powered by neutrinos.

00:00:32 --> 00:00:34 And, uh, Colin is asking about time

00:00:34 --> 00:00:37 dilation. So plenty to talk about on this Q

00:00:37 --> 00:00:40 and A edition of Space nuts. Stick

00:00:40 --> 00:00:40 around.

00:00:40 --> 00:00:43 Professor Fred Watson: 15 seconds. Guidance is internal.

00:00:43 --> 00:00:45 10, 9.

00:00:45 --> 00:00:47 Ignition sequence start.

00:00:47 --> 00:00:48 Professor Fred Watson: Space nuts.

00:00:48 --> 00:00:50 Professor Fred Watson: 5, 4, 3. 2. 1, 2, 3, 4,

00:00:51 --> 00:00:53 5, 5, 4, 3, 2, 1.

00:00:53 --> 00:00:54 Andrew Dunkley: Space nuts.

00:00:54 --> 00:00:56 Professor Fred Watson: Astronauts report it feels good.

00:00:56 --> 00:00:59 Andrew Dunkley: And he's back again to, uh, solve all those

00:00:59 --> 00:01:01 riddles for us. It's Professor Fred Watson

00:01:01 --> 00:01:03 Watson, astronomer at large. Hello, Fre.

00:01:04 --> 00:01:05 Professor Fred Watson: How are you doing, Andrew?

00:01:05 --> 00:01:08 Andrew Dunkley: I'm doing well. You looking rather, um,

00:01:08 --> 00:01:08 um.

00:01:09 --> 00:01:09 Professor Fred Watson: Cold.

00:01:10 --> 00:01:13 Andrew Dunkley: Yes. Maybe. Yeah, we had

00:01:13 --> 00:01:15 a really good warm spell there for a while

00:01:15 --> 00:01:17 and then it just petered out and we're back

00:01:17 --> 00:01:20 to some quite chilly weather. By

00:01:20 --> 00:01:22 the time this podcast comes out, it could be

00:01:22 --> 00:01:25 back to warm again. It's

00:01:25 --> 00:01:27 that time of year where we've got the tug of

00:01:27 --> 00:01:30 war between winter trying to hang on and

00:01:30 --> 00:01:32 spring trying to take over. And so,

00:01:33 --> 00:01:34 uh, you get a little warm snap and then it's

00:01:34 --> 00:01:36 cold again and then you another warm snap and

00:01:36 --> 00:01:38 then one day it just stays warm and then it

00:01:38 --> 00:01:40 gets hot, hot, hot. And then the opposite

00:01:40 --> 00:01:43 happens going into autumn or fall or

00:01:43 --> 00:01:45 whatever, wherever you're from. And however

00:01:45 --> 00:01:47 you say it. But, um, yeah, right now we're

00:01:47 --> 00:01:50 into spring, uh, very windy

00:01:50 --> 00:01:52 weather this time of year out our way.

00:01:52 --> 00:01:54 Nothing to do with actual wind. It's just so

00:01:54 --> 00:01:56 many people sneezing. You just, you know,

00:01:57 --> 00:01:58 volatile environment.

00:01:59 --> 00:01:59 Professor Fred Watson: Yeah.

00:01:59 --> 00:02:01 Professor Fred Watson: Ah, did you, um, you were going to try and

00:02:01 --> 00:02:03 get some shots of, uh, pollen?

00:02:04 --> 00:02:06 Andrew Dunkley: I did try and so far I've failed.

00:02:06 --> 00:02:07 Professor Fred Watson: Okay.

00:02:07 --> 00:02:09 Andrew Dunkley: I haven't been, uh, but see, last time I got

00:02:09 --> 00:02:12 the pollen, uh, corona photo, I was

00:02:12 --> 00:02:15 using an older model phone and I've got

00:02:15 --> 00:02:17 a feeling that the new phone

00:02:17 --> 00:02:19 compensates and actually stops me from

00:02:19 --> 00:02:20 getting the shot.

00:02:21 --> 00:02:22 Professor Fred Watson: Yeah.

00:02:22 --> 00:02:24 Andrew Dunkley: Ah, but I'll give it another try. Uh, I might

00:02:24 --> 00:02:26 have been too early. Cause the best time is

00:02:26 --> 00:02:27 mid afternoon, isn't it?

00:02:27 --> 00:02:29 Professor Fred Watson: Probably, yeah. Uh, you should be able to see

00:02:29 --> 00:02:30 it with the naked eye and that should tell

00:02:30 --> 00:02:33 you what your, um, phone is likely

00:02:33 --> 00:02:34 to pick up.

00:02:34 --> 00:02:36 Andrew Dunkley: A good friend of mine once told me, though,

00:02:36 --> 00:02:38 never to look at the sun.

00:02:38 --> 00:02:41 Professor Fred Watson: Uh, indeed, I tell people that all the time.

00:02:41 --> 00:02:43 But that's why what you do is you get the sun

00:02:43 --> 00:02:45 behind a wall or a building or something,

00:02:45 --> 00:02:48 just enough that you can see the immediate

00:02:48 --> 00:02:50 sky around it and that's where you might see

00:02:50 --> 00:02:52 these colour bands. And just in case any of

00:02:52 --> 00:02:54 our listeners wonder what we're talking

00:02:54 --> 00:02:56 about, um, pollen, uh,

00:02:56 --> 00:02:58 particles in the atmosphere. Because there

00:02:58 --> 00:03:00 are many, many millions of them and they're

00:03:00 --> 00:03:03 all of a uniform size, they have an effect on

00:03:03 --> 00:03:05 light called diffraction, uh, and that

00:03:06 --> 00:03:08 you can get coloured rings around the sun

00:03:08 --> 00:03:11 caused by the diffracting effect of these

00:03:11 --> 00:03:14 pollen, uh, uh, particles. And that's

00:03:14 --> 00:03:15 what Andrew's looked for. I've seen them in

00:03:15 --> 00:03:18 Coonabarabran on occasion when I used to live

00:03:18 --> 00:03:20 out there. We tend not to see them in Sydney

00:03:20 --> 00:03:22 because the air is probably not

00:03:22 --> 00:03:24 Andrew Dunkley: clear enough because there's more pollution

00:03:24 --> 00:03:24 in

00:03:24 --> 00:03:27 Professor Fred Watson: the air than pollens. Yes, there is. Pollen

00:03:27 --> 00:03:28 pollination.

00:03:28 --> 00:03:31 Andrew Dunkley: Yeah, yeah. It's quite

00:03:31 --> 00:03:34 spectacular though. Yes, I think

00:03:34 --> 00:03:36 we talked about it on an episode and I said,

00:03:36 --> 00:03:38 okay, um, challenge acceptance, and went

00:03:38 --> 00:03:40 outside, took one photo and got it.

00:03:40 --> 00:03:42 Professor Fred Watson: Yes, yes, that's right.

00:03:42 --> 00:03:45 Andrew Dunkley: Proving more difficult this time. Let's get

00:03:45 --> 00:03:46 into our questions.

00:03:46 --> 00:03:48 Uh, this first one comes from Larry.

00:03:49 --> 00:03:51 Professor Fred Watson: Hello, Fred Watson and Andrew.

00:03:53 --> 00:03:55 This is Larry from, um, York,

00:03:56 --> 00:03:57 Nebraska, that is.

00:03:59 --> 00:04:02 I've been listening to your podcast

00:04:03 --> 00:04:05 almost continually for months.

00:04:07 --> 00:04:10 Heard an old edition

00:04:10 --> 00:04:11 talking about

00:04:14 --> 00:04:14 Speaker D: using,

00:04:14 --> 00:04:17 Professor Fred Watson: uh, the gravitational boost

00:04:17 --> 00:04:18 around planets,

00:04:20 --> 00:04:22 particularly Pepe

00:04:22 --> 00:04:25 Colombo. Fred Watson

00:04:25 --> 00:04:28 said that, uh, had to

00:04:28 --> 00:04:30 use, uh, nine booths to get

00:04:31 --> 00:04:34 the BP Columbo spacecraft to

00:04:35 --> 00:04:37 speed up to the speed of

00:04:37 --> 00:04:40 Mercury. However, from

00:04:40 --> 00:04:43 previous podcasts it seems

00:04:43 --> 00:04:46 the more you speed up the orbital

00:04:46 --> 00:04:49 velocity, the further away from the

00:04:49 --> 00:04:50 sun you get. So don't you have to

00:04:51 --> 00:04:52 use the

00:04:54 --> 00:04:56 gravitational wells to slow down

00:04:58 --> 00:05:00 to get to Mercury? Because Mercury's

00:05:00 --> 00:05:02 orbital velocity should be a whole lot less

00:05:02 --> 00:05:05 than Earth's. Thank you.

00:05:06 --> 00:05:09 Andrew Dunkley: Thank you, Larry. And, uh, hope all is well

00:05:09 --> 00:05:12 in wonderful Nebraska. Um,

00:05:12 --> 00:05:14 yeah, he brings up an interesting point. Uh,

00:05:15 --> 00:05:17 maybe we can discuss that after we break the

00:05:17 --> 00:05:20 news about BepiColombo. The

00:05:20 --> 00:05:23 BepiColombo mission to Mercury. And

00:05:23 --> 00:05:26 we did talk about how it had to do,

00:05:26 --> 00:05:29 um, quite a bit of manoeuvring, um, to,

00:05:29 --> 00:05:32 to achieve the velocity it required. You

00:05:32 --> 00:05:33 might remind us about that, Fred Watson, and

00:05:33 --> 00:05:36 then tell us, um, what's happening now.

00:05:36 --> 00:05:39 Professor Fred Watson: Uh, yes, so, uh, BepiColombo,

00:05:39 --> 00:05:42 a joint, um, ESA,

00:05:42 --> 00:05:45 uh, JAXA mission, I think. Japanese

00:05:45 --> 00:05:48 Aerospace Exploration Agency.

00:05:48 --> 00:05:51 Um, eight years it's been on

00:05:51 --> 00:05:54 its way so far and ah,

00:05:54 --> 00:05:57 there have been nine, I think I'm right, nine

00:05:57 --> 00:06:00 gravity assists, one of Earth, two of

00:06:00 --> 00:06:01 Venus and six of Mercury itself.

00:06:03 --> 00:06:05 Uh, and the reason why it's in the news at

00:06:05 --> 00:06:08 the moment is because um, the

00:06:08 --> 00:06:11 spacecraft has separated

00:06:11 --> 00:06:14 from its um, something called

00:06:14 --> 00:06:17 the MTM M M which

00:06:17 --> 00:06:20 is the uh,

00:06:21 --> 00:06:24 Mercury Transfer Module. In other

00:06:24 --> 00:06:26 words it's almost like a service module

00:06:26 --> 00:06:28 that's been uh, attached to the spacecraft.

00:06:28 --> 00:06:31 It's got solar panels, it's got you know,

00:06:31 --> 00:06:33 various uh, um, uh,

00:06:33 --> 00:06:36 feeds uh, on board for

00:06:36 --> 00:06:38 the requisites of the spacecraft itself

00:06:39 --> 00:06:41 that has now basically been jettisoned.

00:06:42 --> 00:06:45 Uh, and so BepiColombo is on its

00:06:45 --> 00:06:47 own as it spirals

00:06:47 --> 00:06:50 down towards the planet

00:06:50 --> 00:06:53 Mercury to eventually go into orbit

00:06:53 --> 00:06:53 around Mercury.

00:06:53 --> 00:06:55 Andrew Dunkley: And seeing they've now separated, uh, the

00:06:55 --> 00:06:57 lawyers will be deciding who gets what

00:06:57 --> 00:06:59 Professor Fred Watson: assets, who gets what. Yeah,

00:07:00 --> 00:07:03 indeed, that's right. Um, but let's just

00:07:03 --> 00:07:05 go to um, Larry's question. Uh,

00:07:06 --> 00:07:08 Larry's. You're

00:07:08 --> 00:07:11 absolutely right. This is something

00:07:11 --> 00:07:14 I think it does all our heads in that

00:07:17 --> 00:07:19 ah, if you've got a spacecraft in orbit

00:07:19 --> 00:07:21 around something and you speed it up,

00:07:22 --> 00:07:25 what happens is it goes to a higher orbit but

00:07:25 --> 00:07:28 it slows down that um,

00:07:28 --> 00:07:30 speed the bottom line. And the

00:07:30 --> 00:07:33 reverse is true with BepiColombo

00:07:33 --> 00:07:36 going to Mercury. So um,

00:07:37 --> 00:07:39 remembering that the Earth's orbital velocity

00:07:40 --> 00:07:42 around the sun

00:07:42 --> 00:07:44 is 30 kilometres per second,

00:07:45 --> 00:07:48 uh Mercury has an orbital

00:07:48 --> 00:07:51 velocity which is in the

00:07:51 --> 00:07:53 region of 50 kilometres per second.

00:07:54 --> 00:07:57 M uh because it's nearer the sun it

00:07:57 --> 00:07:59 needs a higher velocity to stop it from

00:07:59 --> 00:08:02 falling into the so 50

00:08:02 --> 00:08:04 kilometres per second is its speed. So in

00:08:04 --> 00:08:07 that respect BepiColombo

00:08:07 --> 00:08:10 is catching up uh in terms of

00:08:10 --> 00:08:13 speed uh with Mercury.

00:08:13 --> 00:08:16 But to do that you slow it

00:08:16 --> 00:08:19 down, you have to shed the Earth's

00:08:19 --> 00:08:22 uh, orbital velocity to push the

00:08:22 --> 00:08:24 spacecraft in towards the sun which

00:08:24 --> 00:08:27 speeds it up uh, so that it would be

00:08:27 --> 00:08:29 travelling faster than the Earth. If I can

00:08:29 --> 00:08:31 put it that way. It's all about the balance

00:08:31 --> 00:08:34 between gravity and velocity.

00:08:34 --> 00:08:36 Uh, I'm probably not making this sound very

00:08:36 --> 00:08:38 clear but the bottom line is that it's taken

00:08:38 --> 00:08:41 those uh, nine gravity assists to get

00:08:41 --> 00:08:44 from 30 kilometres per second going around

00:08:44 --> 00:08:47 the Earth to roughly 50

00:08:47 --> 00:08:49 kilometres per second average speed of

00:08:49 --> 00:08:52 Mercury. I think it gets significantly higher

00:08:52 --> 00:08:53 and lower because Mercury's got quite an

00:08:53 --> 00:08:56 elliptical orbit. Um, believe Its maximum

00:08:56 --> 00:08:59 is 59 kilometres per second when it's closest

00:08:59 --> 00:09:01 to the sun. So you're talking about a

00:09:01 --> 00:09:03 significant increase in velocity which

00:09:04 --> 00:09:07 achieved by slowing the spacecraft down so it

00:09:07 --> 00:09:10 falls in towards the Inner solar system. Does

00:09:10 --> 00:09:11 that make sense?

00:09:11 --> 00:09:14 Andrew Dunkley: Yeah, I think we talked about, uh, when this

00:09:14 --> 00:09:16 first came up, we talked about how much more

00:09:16 --> 00:09:18 difficult it is to go towards the

00:09:18 --> 00:09:21 centre of our solar system than it is to go

00:09:21 --> 00:09:24 Professor Fred Watson: outwards in that regard. It is, that's

00:09:24 --> 00:09:24 correct, yes.

00:09:24 --> 00:09:25 Professor Fred Watson: Yeah.

00:09:25 --> 00:09:27 Andrew Dunkley: So there's a lot of mathematicians, um,

00:09:28 --> 00:09:30 at work trying to figure this one out.

00:09:31 --> 00:09:33 Um, um, you know, taking into account

00:09:33 --> 00:09:36 orbital mechanics, M and the, uh,

00:09:36 --> 00:09:38 everything that goes into it, uh, it's quite

00:09:38 --> 00:09:41 an amazing feat, to be honest, to uh, to

00:09:41 --> 00:09:43 come up with this. And yet you think a jump

00:09:43 --> 00:09:46 of only 20 kilometres per second, 30 to 50,

00:09:46 --> 00:09:48 wouldn't. It doesn't sound all that

00:09:48 --> 00:09:50 difficult. But when you look at what they've

00:09:50 --> 00:09:52 actually had to do to achieve it.

00:09:52 --> 00:09:52 Professor Fred Watson: That's right.

00:09:52 --> 00:09:53 Andrew Dunkley: Quite extraordinary.

00:09:53 --> 00:09:56 Professor Fred Watson: It is, it's, it's, it is a significant amount

00:09:57 --> 00:09:58 when you think about it. You know, you're

00:09:59 --> 00:10:02 like that 20 kilometres per second, uh,

00:10:03 --> 00:10:06 is, it's. I think it was about the

00:10:06 --> 00:10:09 same orbital speed that, um, New Horizons

00:10:09 --> 00:10:10 was launched at when it was one of the

00:10:10 --> 00:10:12 fastest spacecraft ever launched. I think it

00:10:12 --> 00:10:14 was 23 kilometres per second it had. So

00:10:14 --> 00:10:17 it's a not insignificant jump in velocity.

00:10:18 --> 00:10:21 Andrew Dunkley: It just takes a lot of manoeuvring to make it

00:10:21 --> 00:10:21 happen.

00:10:21 --> 00:10:23 Professor Fred Watson: Indeed, yeah, that's right.

00:10:23 --> 00:10:26 Andrew Dunkley: There you go. Larry explained and still, um,

00:10:26 --> 00:10:27 scratching my head.

00:10:29 --> 00:10:32 Thanks for the question. Um, this is Space

00:10:32 --> 00:10:34 Nuts with Andrew Dunkley and Professor

00:10:34 --> 00:10:35 Fred Watson Watson. It's a Q and A edition.

00:10:37 --> 00:10:39 Professor Fred Watson: I believe that this nation should commit

00:10:39 --> 00:10:42 Andrew Dunkley: itself to achieving the goal,

00:10:42 --> 00:10:43 before this

00:10:43 --> 00:10:45 Professor Fred Watson: decade is out, of landing a man

00:10:45 --> 00:10:48 Professor Fred Watson: on the moon and returning him safely to the

00:10:48 --> 00:10:48 Earth.

00:10:48 --> 00:10:51 Andrew Dunkley: These nuts. Now, next question comes from

00:10:51 --> 00:10:54 Eduardo. I hope I'm pronouncing that

00:10:54 --> 00:10:57 correctly. Um, he says, given

00:10:57 --> 00:11:00 that neutrinos are the second most abundant

00:11:00 --> 00:11:03 subatopic particle, just after photons.

00:11:03 --> 00:11:06 Uh, but contrary to photons, they don't seem,

00:11:06 --> 00:11:09 seem to interact that much with matter. Do

00:11:09 --> 00:11:11 black holes swallow neutrinos

00:11:12 --> 00:11:14 or do they just pass through them? Are

00:11:14 --> 00:11:17 neutrinos affected by gravity at all?

00:11:18 --> 00:11:21 Professor Fred Watson: Um, so yes, they are. Uh, and

00:11:21 --> 00:11:24 I mean in the, you know, light is as. Well,

00:11:24 --> 00:11:25 of course, light, that's the thing about a

00:11:25 --> 00:11:28 black hole, um, uh, won't even

00:11:28 --> 00:11:31 allow the release of light beyond the event

00:11:31 --> 00:11:34 horizon. Uh, and the same is true

00:11:34 --> 00:11:36 with neutrinos. So neutrinos,

00:11:37 --> 00:11:39 they can't pass through a black hole. Uh, if

00:11:39 --> 00:11:41 they cross the event horizon, they're

00:11:41 --> 00:11:44 trapped, uh, just like particles of

00:11:44 --> 00:11:46 light. Uh, um,

00:11:47 --> 00:11:50 uh, it is a bit weird with

00:11:50 --> 00:11:53 neutrinos because they Exactly. Um, as

00:11:53 --> 00:11:56 Eduardo says, they pass through normal matter

00:11:56 --> 00:11:58 very easily. They don't interact much with

00:11:58 --> 00:12:01 normal matter. Uh, but nevertheless

00:12:01 --> 00:12:03 gravity and the curvature of space time,

00:12:03 --> 00:12:05 which is really what we're talking about with

00:12:05 --> 00:12:07 a black. Black hole, uh, they affect them

00:12:07 --> 00:12:09 just the same as everything else.

00:12:09 --> 00:12:10 Speaker D: Hmm.

00:12:10 --> 00:12:12 Andrew Dunkley: Simple as that. It wouldn't be too much. That

00:12:12 --> 00:12:14 would not be affected by gravity.

00:12:15 --> 00:12:18 Professor Fred Watson: Yes, that's right. Uh, we think dark

00:12:18 --> 00:12:20 matter is too. Well, we know dark matter is.

00:12:20 --> 00:12:21 That's the only way we know it exists. So.

00:12:21 --> 00:12:23 Andrew Dunkley: Yes, well, it seems to clump in higher

00:12:24 --> 00:12:26 gravitational fields, doesn't it?

00:12:26 --> 00:12:27 Professor Fred Watson: That's correct, yes.

00:12:27 --> 00:12:29 Andrew Dunkley: Um, even though we don't really understand

00:12:29 --> 00:12:31 it, although we do think they may have

00:12:32 --> 00:12:34 identified it recently. Uh, I think we talked

00:12:34 --> 00:12:37 about that last episode. So, um,

00:12:37 --> 00:12:39 yeah, we're slowly chipping away at the

00:12:39 --> 00:12:42 mystery of dark matter, hopefully. So

00:12:42 --> 00:12:44 he said that, um, neutrinos are the second

00:12:44 --> 00:12:47 most abundant subatopic particle. Is that

00:12:47 --> 00:12:48 right?

00:12:48 --> 00:12:50 Professor Fred Watson: Um, I'd need to cheque that, but I think it's

00:12:50 --> 00:12:52 probably right. Yes. Uh,

00:12:53 --> 00:12:55 I think that's ah, a correct statement.

00:12:56 --> 00:12:58 Andrew Dunkley: Do we know what they're supposed to do?

00:12:58 --> 00:12:59 What's their function?

00:13:00 --> 00:13:03 Professor Fred Watson: Well, yeah, they're um, byproduct

00:13:03 --> 00:13:05 of, uh, nuclear reactions.

00:13:06 --> 00:13:09 And they are prolific, as

00:13:09 --> 00:13:11 Eduardo suggested. So, um,

00:13:11 --> 00:13:14 with um, for example, the nuclear reactions

00:13:14 --> 00:13:17 that power the sun, uh, the

00:13:17 --> 00:13:20 um, what's it called, the fusion

00:13:20 --> 00:13:23 reactions, uh, it's got a name.

00:13:23 --> 00:13:24 Proton. Proton reaction. There's several

00:13:24 --> 00:13:27 different ones anyway. They not only

00:13:27 --> 00:13:30 produce, uh, helium from hydrogen,

00:13:30 --> 00:13:32 uh, but the energy that they produce, uh, is

00:13:32 --> 00:13:35 in gamma rays and in neutrinos as well.

00:13:36 --> 00:13:36 Professor Fred Watson: There you, um, go.

00:13:37 --> 00:13:38 Andrew Dunkley: Fascinating.

00:13:39 --> 00:13:41 Um, Eduardo, that's um, about all we can tell

00:13:41 --> 00:13:43 you about that, but thanks for the question.

00:13:43 --> 00:13:44 Lovely to hear from you. We're whipping m

00:13:45 --> 00:13:46 through them, Fred Watson. We are.

00:13:48 --> 00:13:50 Uh, this is Space Nuts, a Q and A edition

00:13:50 --> 00:13:52 with Andrew Nunkley and Professor Fred Watson

00:13:52 --> 00:13:53 Watson.

00:13:56 --> 00:13:58 Professor Fred Watson: Three, two, one.

00:13:59 --> 00:14:01 Andrew Dunkley: Space Nuts. Uh, our next question

00:14:02 --> 00:14:04 comes from Shumo, who says. Hi, Fred Watson

00:14:04 --> 00:14:07 and Andrew. Another alien communication

00:14:07 --> 00:14:10 question. SETI understandably concentrates on

00:14:10 --> 00:14:13 radio and optical signals, but are we being

00:14:13 --> 00:14:15 too anthropo. I can't

00:14:15 --> 00:14:18 say it. Anthropocentric

00:14:19 --> 00:14:21 about the carrier. Couldn't, uh, advanced

00:14:21 --> 00:14:24 civilization use high energy gamma rays or

00:14:24 --> 00:14:27 even neutrinos as an interstellar beacon,

00:14:27 --> 00:14:30 encoding information in the timing or energy

00:14:30 --> 00:14:33 of individual event. Example, repeated gamma

00:14:33 --> 00:14:36 ray or neutrino events from the same point

00:14:36 --> 00:14:38 in the sky following the prime numbers would

00:14:38 --> 00:14:41 be very difficult to explain. Naturally,

00:14:41 --> 00:14:44 given that, uh, uh, we

00:14:44 --> 00:14:46 already have gamma ray and neutrino

00:14:46 --> 00:14:48 observatories watching the sky. Has anyone

00:14:48 --> 00:14:50 systematically searched their data for

00:14:50 --> 00:14:53 mathematically structured patterns that might

00:14:53 --> 00:14:56 be artificial? That comes from Shumo in

00:14:56 --> 00:14:58 Oxford in the uk. That's a really good

00:14:58 --> 00:15:00 question. Like that's out of the box. Isn't.

00:15:01 --> 00:15:04 Professor Fred Watson: Um, is a good question. And

00:15:05 --> 00:15:07 in a way, um, the answer lies in

00:15:08 --> 00:15:11 the fact that uh, when gamma ray bursts

00:15:11 --> 00:15:14 were first detected, uh, which you'll

00:15:14 --> 00:15:16 remember were detected by spacecraft

00:15:16 --> 00:15:18 satellites that had been launched

00:15:18 --> 00:15:21 specifically to look for evidence of breaches

00:15:21 --> 00:15:23 of the Nuclear Test Ban Treaty, the

00:15:23 --> 00:15:26 Atmospheric Nuclear Test Ban Treaty. That's

00:15:26 --> 00:15:28 what they were built for. They didn't see any

00:15:28 --> 00:15:31 nuclear tests, but uh, they

00:15:31 --> 00:15:34 saw these things coming from the sky, uh,

00:15:34 --> 00:15:36 bursts of radiation. So the first thing you

00:15:36 --> 00:15:38 think of when you see something like that is,

00:15:38 --> 00:15:40 is this a SETI signal,

00:15:41 --> 00:15:43 uh, or something artificial now,

00:15:43 --> 00:15:46 um, with gamma rays and indeed neutrino,

00:15:46 --> 00:15:49 uh, radiation. I guess

00:15:49 --> 00:15:52 you would tend to put that,

00:15:52 --> 00:15:55 to put an artificial origin fairly

00:15:55 --> 00:15:58 low on the list of, of candidate,

00:15:58 --> 00:16:01 um, reasons why these things are flying

00:16:01 --> 00:16:04 through space. Because they're very, very

00:16:04 --> 00:16:07 high, energetic, high energy, um,

00:16:07 --> 00:16:10 carriers. Uh, we're talking about a high

00:16:10 --> 00:16:13 energy universe here. Having um,

00:16:14 --> 00:16:16 said that, I recently wrote the

00:16:16 --> 00:16:19 foreword for a book by a group of

00:16:19 --> 00:16:21 colleagues at the Western Sydney University,

00:16:22 --> 00:16:23 which is called High Energy

00:16:23 --> 00:16:26 Astrobiology. Uh, and there you

00:16:26 --> 00:16:29 have it. The link between high energy

00:16:30 --> 00:16:32 physics phenomena and the science

00:16:32 --> 00:16:35 of the origin and evolution of life.

00:16:36 --> 00:16:38 Uh, and so I can't remember actually the

00:16:38 --> 00:16:41 details of the chapters. Um, uh, I

00:16:41 --> 00:16:43 do have a copy of the book which I looked

00:16:43 --> 00:16:45 through and enjoyed reading. Um,

00:16:46 --> 00:16:49 but uh, I can't remember the details. But

00:16:49 --> 00:16:52 um, I wouldn't mind betting that somewhere in

00:16:52 --> 00:16:55 there somebody is basically

00:16:55 --> 00:16:58 highlighting essentially the same question

00:16:58 --> 00:16:59 that Schumach has raised here.

00:17:01 --> 00:17:01 So.

00:17:01 --> 00:17:03 Andrew Dunkley: Yeah, I imagine so. But

00:17:04 --> 00:17:06 surely there'd be easier ways to send a

00:17:06 --> 00:17:07 message if you were.

00:17:07 --> 00:17:07 Professor Fred Watson: Yeah.

00:17:07 --> 00:17:09 Professor Fred Watson: Uh, rather than blowing up a planet or

00:17:09 --> 00:17:11 something like that, which is, you know, the

00:17:11 --> 00:17:12 kind of energies that we're talking about

00:17:12 --> 00:17:13 here. Yes.

00:17:13 --> 00:17:16 Andrew Dunkley: No, it kind of worked for. Ah, the Empire

00:17:16 --> 00:17:16 didn't.

00:17:19 --> 00:17:21 Professor Fred Watson: Depends on whose side you're on really.

00:17:21 --> 00:17:23 Andrew Dunkley: Yes, but,

00:17:23 --> 00:17:26 um. Would lasers be feasible over, um,

00:17:26 --> 00:17:27 parsecs?

00:17:28 --> 00:17:31 Professor Fred Watson: Yeah, they are. I mean, and so. Yes. But you

00:17:31 --> 00:17:34 know, in that regard I, uh, guess, um.

00:17:34 --> 00:17:37 Uh, you know, Shuma's already raised

00:17:38 --> 00:17:40 the issue that um, we've got,

00:17:41 --> 00:17:44 uh, the idea of optical communications

00:17:44 --> 00:17:46 as part and parcel of our

00:17:46 --> 00:17:48 retinue of researchers,

00:17:50 --> 00:17:52 uh, when it comes to possible

00:17:52 --> 00:17:54 SETI signals. Um,

00:17:55 --> 00:17:58 and exactly as

00:17:58 --> 00:18:00 Schumacher says, uh, SETI understandably

00:18:00 --> 00:18:02 concentrates on radio and optical signals.

00:18:02 --> 00:18:04 And yeah, that's why, because they're going

00:18:04 --> 00:18:07 to be the easiest to produce. Very much so.

00:18:07 --> 00:18:09 Optical signals I think have been neglected a

00:18:09 --> 00:18:12 bit in comparison with radio signals.

00:18:13 --> 00:18:15 But that is coming to an end because,

00:18:17 --> 00:18:20 uh, the latest instruments

00:18:20 --> 00:18:22 that we have, looking at the optical sky,

00:18:22 --> 00:18:24 optical and near infrared sky, and I'm

00:18:24 --> 00:18:27 thinking particularly of the Vera C. Rubin

00:18:27 --> 00:18:29 Observatory. Now it finds transient

00:18:29 --> 00:18:32 events, uh, millions per

00:18:32 --> 00:18:35 night. By transient events, I mean things

00:18:35 --> 00:18:37 that come and go in the dark. And of course

00:18:37 --> 00:18:40 communication signals would fall into that

00:18:40 --> 00:18:40 category.

00:18:40 --> 00:18:41 Speaker D: Yeah.

00:18:41 --> 00:18:44 Andrew Dunkley: When I was doing the research for my

00:18:45 --> 00:18:47 new sci fi trilogy, um,

00:18:48 --> 00:18:50 the first book in the series is called the

00:18:50 --> 00:18:52 Signal. And I did

00:18:53 --> 00:18:55 quite um, a bit of research on what

00:18:56 --> 00:18:58 signal would be likely to be received

00:18:59 --> 00:19:02 on Earth by an alien intelligence.

00:19:02 --> 00:19:05 And it basically came down to the signals

00:19:05 --> 00:19:07 we use every day on our own planet. The

00:19:07 --> 00:19:09 signals in the hydrogen line,

00:19:10 --> 00:19:13 1.4 to, to 1.66

00:19:13 --> 00:19:16 gigahertz, um, 14, 20 megahertz

00:19:16 --> 00:19:18 range that AM radio

00:19:18 --> 00:19:21 frequencies basically, um, more or less. Uh,

00:19:21 --> 00:19:24 so that's what I based it on.

00:19:24 --> 00:19:26 Um, but

00:19:28 --> 00:19:31 that's more likely to be the kind of

00:19:31 --> 00:19:33 signal that would be sent by a communicative

00:19:34 --> 00:19:36 intelligence beyond Earth. And

00:19:36 --> 00:19:38 that's where the Drake equation comes in.

00:19:39 --> 00:19:41 Um, I think they're based on an

00:19:41 --> 00:19:43 intelligence that is capable of

00:19:44 --> 00:19:45 communication.

00:19:46 --> 00:19:48 Professor Fred Watson: And you're absolutely right.

00:19:49 --> 00:19:51 Right from the beginning of what you might

00:19:51 --> 00:19:54 call the SETI era, looking for

00:19:54 --> 00:19:56 extraterrestrial intelligence. That

00:19:56 --> 00:19:59 hydrogen line that you've spoken of, 21

00:19:59 --> 00:20:01 centimetre line, to put it in wavelengths

00:20:01 --> 00:20:03 rather than frequency, um,

00:20:04 --> 00:20:06 is what cold hydrogen emits.

00:20:07 --> 00:20:08 So it's the most prolific

00:20:10 --> 00:20:10 Professor Fred Watson: spectral uh,

00:20:11 --> 00:20:13 Professor Fred Watson: line in the whole universe

00:20:14 --> 00:20:16 of any uh, frequency band.

00:20:17 --> 00:20:20 And so um, it is naturally where you would

00:20:20 --> 00:20:22 start thinking about broadcasting if you are

00:20:22 --> 00:20:25 trying to send a signal out, uh, to

00:20:25 --> 00:20:28 another intelligence, which

00:20:28 --> 00:20:31 that's a whole, I guess the whole um,

00:20:32 --> 00:20:34 proposition of SETI that uh, the

00:20:35 --> 00:20:37 intelligent species out there might want to

00:20:37 --> 00:20:39 communicate. And how they're going to do it.

00:20:39 --> 00:20:41 Well, they're going to use the spectral line

00:20:41 --> 00:20:43 that we're looking for anyway because that's

00:20:43 --> 00:20:45 something we're using to m. Map the universe.

00:20:45 --> 00:20:46 Speaker D: Yeah.

00:20:46 --> 00:20:48 Andrew Dunkley: Was the wow. Signal in that frequency range?

00:20:48 --> 00:20:50 Professor Fred Watson: I think I, uh, think it was, yes. Yeah, I

00:20:50 --> 00:20:51 think it was.

00:20:51 --> 00:20:53 Andrew Dunkley: And that, that came from the um,

00:20:54 --> 00:20:57 Sagittarius constellation region of

00:20:57 --> 00:21:00 spaces. Because I researched that as well

00:21:01 --> 00:21:04 off the top of my head. Um, they

00:21:04 --> 00:21:06 have actually studied that part of the

00:21:06 --> 00:21:08 universe and they at this moment cannot find

00:21:08 --> 00:21:11 anything to suggest that it was an artificial

00:21:11 --> 00:21:14 uh, signal. But

00:21:14 --> 00:21:16 they still haven't figured that one out, have

00:21:16 --> 00:21:16 they?

00:21:16 --> 00:21:19 Professor Fred Watson: No, there have been a few ideas like radio,

00:21:19 --> 00:21:21 uh, emission from comets. That was one. Uh.

00:21:21 --> 00:21:23 Cause I think there were comets in the sky at

00:21:23 --> 00:21:25 the time. But yeah,

00:21:26 --> 00:21:28 it's still an open question.

00:21:29 --> 00:21:32 Andrew Dunkley: Yeah, I guess so. All right, um, that's

00:21:32 --> 00:21:34 a great question. Thanks uh, Shumo, for

00:21:34 --> 00:21:37 sending it in. Um, but uh, yeah, there's

00:21:37 --> 00:21:40 probably easier ways to do things and uh, if

00:21:40 --> 00:21:42 you're going to send a signal to an

00:21:42 --> 00:21:45 alien civilization, you probably want them to

00:21:45 --> 00:21:48 be able to figure it out rather

00:21:48 --> 00:21:50 than send them something complex and they go,

00:21:50 --> 00:21:53 no, no, I don't know what that was. Um, let's

00:21:53 --> 00:21:56 go to our final question from Colin.

00:21:56 --> 00:21:58 Speaker D: Hello, Andrew and Fred Watson.

00:21:58 --> 00:22:00 Colin from Adelaide. I love the

00:22:00 --> 00:22:03 science fiction movie project Hail Mary,

00:22:03 --> 00:22:06 which I've seen twice. But I'm still quite

00:22:06 --> 00:22:09 confused about the time dilation effects. In

00:22:09 --> 00:22:11 the movie. RYLAND Grace travels

00:22:11 --> 00:22:14 12 light years to his destination

00:22:15 --> 00:22:18 at ah, Tau Ceti in four years

00:22:18 --> 00:22:20 and eight months. How can this be? The

00:22:20 --> 00:22:23 Beatles powered by the astrophage

00:22:23 --> 00:22:26 fuel carrying Tau Moeba, the

00:22:26 --> 00:22:29 solution to the astrophage problem with

00:22:29 --> 00:22:32 the sun reach Earth even quicker than.

00:22:32 --> 00:22:35 Than this. How can that be? And lastly,

00:22:35 --> 00:22:38 if Ryan Grace had returned

00:22:38 --> 00:22:41 to Earth, how much younger would he be

00:22:41 --> 00:22:44 than those he left behind? Very confusing.

00:22:44 --> 00:22:46 I hope you can help. Thank you. Love the

00:22:46 --> 00:22:47 podcast.

00:22:48 --> 00:22:51 Andrew Dunkley: Yeah, thanks, Colin. Um, I've seen the movie

00:22:51 --> 00:22:53 a couple of times myself and I've got to

00:22:53 --> 00:22:56 confess that I'm as confused as Colin

00:22:56 --> 00:22:59 in regard to the distances travelled and how

00:22:59 --> 00:23:02 fast they achieved it. Even though they came

00:23:02 --> 00:23:05 up with a new drive concept that

00:23:05 --> 00:23:08 um, even that I had trouble getting

00:23:08 --> 00:23:10 my head around, they, they did explain it and

00:23:10 --> 00:23:13 I just sat there sort of glazed look on

00:23:13 --> 00:23:16 my, on my face. Um, because it

00:23:16 --> 00:23:18 was uh, it was very cleverly done.

00:23:19 --> 00:23:21 But I don't know how they did it.

00:23:22 --> 00:23:25 Someone else might be able to explain uh, it

00:23:25 --> 00:23:28 to me. Um, I suppose we

00:23:28 --> 00:23:31 can tackle the question in two ways. My

00:23:31 --> 00:23:33 answer, Colin, is it's science fiction. You

00:23:33 --> 00:23:36 can do whatever you damn would like. Um,

00:23:36 --> 00:23:38 but that's just, that's the, that's a very

00:23:38 --> 00:23:41 simplistic answer. Um, when I

00:23:41 --> 00:23:44 write my science fiction novels, I

00:23:44 --> 00:23:47 want at least some of it to be as

00:23:47 --> 00:23:50 believable as possible. And so

00:23:50 --> 00:23:52 I'm, I'm in your boat. I want to know how

00:23:52 --> 00:23:55 they did it. Um, the

00:23:55 --> 00:23:56 other, yeah, the other side of it is,

00:23:57 --> 00:24:00 um, that we should

00:24:00 --> 00:24:02 explain time dilation and

00:24:03 --> 00:24:05 see where that falls within the parameters of

00:24:05 --> 00:24:08 the film. You haven't seen it, Fred Watson,

00:24:08 --> 00:24:10 have you? Oh, you have? What did you Think.

00:24:10 --> 00:24:12 Professor Fred Watson: Um, so, uh. Well, I was hoping you'd have the

00:24:12 --> 00:24:15 answer to this question. Not like, because I

00:24:15 --> 00:24:18 did watch it. I watched it on a flight from,

00:24:19 --> 00:24:22 a flight from Sydney to Paris,

00:24:23 --> 00:24:26 um, which uh, gave

00:24:26 --> 00:24:29 me enough time to watch the movie uh,

00:24:30 --> 00:24:32 thoroughly but still,

00:24:33 --> 00:24:35 I was still vaguely half asleep at the time.

00:24:35 --> 00:24:38 So um, and look, so I can't,

00:24:38 --> 00:24:41 I'm, I can't comment on those um, those uh,

00:24:41 --> 00:24:44 values uh, that um, that uh, Colin's

00:24:44 --> 00:24:45 given us. But.

00:24:45 --> 00:24:47 Andrew Dunkley: Well I, I got it. I've just done a quick

00:24:47 --> 00:24:50 search and. Okay, so the, the destination

00:24:50 --> 00:24:53 for our hero of the movie uh,

00:24:53 --> 00:24:56 was the star system Tau Ceti which was,

00:24:56 --> 00:24:59 is 11.9 light years from

00:24:59 --> 00:25:01 Earth. To get there.

00:25:02 --> 00:25:04 Um, the spacecraft was

00:25:04 --> 00:25:07 powered by a microorganism called

00:25:07 --> 00:25:10 Astrophage that converts mass into pure

00:25:10 --> 00:25:13 energy and that enabled

00:25:13 --> 00:25:15 the constant acceleration of

00:25:15 --> 00:25:18 1.5 g for the first half of the trip

00:25:18 --> 00:25:21 and then it flips and decelerates at 1.5 g

00:25:21 --> 00:25:23 for the second half of the trip. Its peak

00:25:23 --> 00:25:25 velocity was roughly

00:25:25 --> 00:25:28 92% the speed of light. Okay.

00:25:29 --> 00:25:31 If that's the case, travelling

00:25:31 --> 00:25:34 11.9 light years would take

00:25:34 --> 00:25:37 longer than 11.9 years and

00:25:37 --> 00:25:40 he got there in, I think it was

00:25:40 --> 00:25:43 four years. Uh, uh, that's why

00:25:43 --> 00:25:44 Colin's confused.

00:25:44 --> 00:25:47 Professor Fred Watson: Well, I mean time dilation only works.

00:25:47 --> 00:25:47 Andrew Dunkley: Yes.

00:25:48 --> 00:25:51 Professor Fred Watson: When you're talking about two separate frames

00:25:51 --> 00:25:52 of reference.

00:25:52 --> 00:25:55 Andrew Dunkley: Well, it's 11.9 light years if

00:25:55 --> 00:25:56 you're staying on Earth.

00:25:56 --> 00:25:56 Professor Fred Watson: Yes.

00:25:57 --> 00:25:59 Andrew Dunkley: When you're travelling it's a different

00:25:59 --> 00:26:00 kettle of fish.

00:26:00 --> 00:26:03 Professor Fred Watson: Yes, that's correct. Um, and so the

00:26:03 --> 00:26:06 time dilation, the time basically

00:26:06 --> 00:26:09 slows down for you as you're travelling

00:26:09 --> 00:26:12 relative to the person back on Earth.

00:26:12 --> 00:26:15 Uh, and so that seems to make sense from

00:26:15 --> 00:26:18 what you were saying that um, the experience

00:26:19 --> 00:26:21 of the astronaut is one

00:26:22 --> 00:26:24 of, in terms of Earth, time is a

00:26:24 --> 00:26:26 shorter time even though as far as the clocks

00:26:26 --> 00:26:28 are concerned they're still ticking at the

00:26:28 --> 00:26:30 same speed for the person who's travelling.

00:26:30 --> 00:26:33 Andrew Dunkley: Yeah. And I uh, must confess that

00:26:33 --> 00:26:35 in doing my research for the book that's

00:26:35 --> 00:26:38 um, the target star that

00:26:38 --> 00:26:41 shall remain nameless in my storey. Otherwise

00:26:41 --> 00:26:43 it gets too predictable.

00:26:44 --> 00:26:44 Professor Fred Watson: Um,

00:26:47 --> 00:26:49 Andrew Dunkley: was a certain distance from Earth

00:26:50 --> 00:26:53 as the crow flies or as the photons

00:26:53 --> 00:26:56 fly, but in travelling there

00:26:56 --> 00:26:59 in a, in a capable vessel,

00:26:59 --> 00:27:02 um, the, the time to get

00:27:02 --> 00:27:05 there was cut. Right. Quite dramatically

00:27:05 --> 00:27:08 but in doing so you didn't age,

00:27:08 --> 00:27:11 but everybody back on Earth did still age

00:27:11 --> 00:27:14 the so many light years. Uh,

00:27:14 --> 00:27:16 and, and that's the quandary, isn't it?

00:27:16 --> 00:27:16 Professor Fred Watson: It's um.

00:27:17 --> 00:27:19 Professor Fred Watson: Well, yes, the Twins paradox, basically.

00:27:19 --> 00:27:20 Andrew Dunkley: Exactly.

00:27:20 --> 00:27:21 Speaker D: Yeah. Yeah.

00:27:21 --> 00:27:24 Andrew Dunkley: So, um, it is a thing and it.

00:27:25 --> 00:27:28 Yeah, the. The traveller doesn't,

00:27:28 --> 00:27:30 um, take that amount of time to get there

00:27:30 --> 00:27:33 because of the fact that they're

00:27:33 --> 00:27:35 moving through space at a. At a high

00:27:35 --> 00:27:37 velocity. And, um.

00:27:39 --> 00:27:42 Yeah, I really

00:27:42 --> 00:27:43 struggle to explain this stuff.

00:27:44 --> 00:27:46 Professor Fred Watson: Well, you should. Yeah. The calculation's

00:27:46 --> 00:27:49 easy. Uh, for time dilation, I've seen

00:27:49 --> 00:27:52 it. 1 over the square root of 1 minus

00:27:52 --> 00:27:54 V squared over C squared. You could do that

00:27:54 --> 00:27:55 in your head, Andrew.

00:27:55 --> 00:27:57 Andrew Dunkley: Yeah, I actually had it written down.

00:27:58 --> 00:28:01 I did have it written down. Yeah. That's the

00:28:01 --> 00:28:03 one. Um, but, yeah, I don't have to.

00:28:04 --> 00:28:06 Professor Fred Watson: Nearly everything in special relativity has

00:28:06 --> 00:28:09 this terminate of 1 over the square root

00:28:09 --> 00:28:12 of 1 minus V squared over C squared. It pops

00:28:12 --> 00:28:14 up everywhere. Time dilation, Lorentz

00:28:14 --> 00:28:17 contraction, all of those things. It's the

00:28:17 --> 00:28:17 same factor.

00:28:19 --> 00:28:22 Andrew Dunkley: Suggest to Colin, um, if he wants to read the

00:28:22 --> 00:28:24 Human Epoch, Part one, uh,

00:28:25 --> 00:28:27 there is an explanation of it in there.

00:28:27 --> 00:28:30 Professor Fred Watson: This is your trilogy. Yes, part one

00:28:30 --> 00:28:32 of the trilogy. I think that's what you

00:28:32 --> 00:28:35 probably should do, Colin. Uh, and then you

00:28:35 --> 00:28:37 can bug Andrew about it.

00:28:38 --> 00:28:40 Andrew Dunkley: Well, I've already had a few people come to

00:28:40 --> 00:28:43 me and say, hang on a minute, hang on

00:28:43 --> 00:28:45 a minute. How did you figure that out?

00:28:45 --> 00:28:48 Professor Fred Watson: As you say, you're a science fiction writer.

00:28:48 --> 00:28:50 You can say whatever you want.

00:28:50 --> 00:28:50 Professor Fred Watson: Yeah.

00:28:50 --> 00:28:52 Andrew Dunkley: But I like. I like to get things right, so.

00:28:52 --> 00:28:54 Professor Fred Watson: Uh. Yeah, well, you should. That's right.

00:28:55 --> 00:28:58 Andrew Dunkley: All right. Uh, Colin, that's a fun question.

00:28:58 --> 00:29:00 And it is a really great film. If.

00:29:00 --> 00:29:03 If you haven't seen it. It's still one of the

00:29:03 --> 00:29:05 top picks on some of those, um, streaming

00:29:05 --> 00:29:07 platforms. Because it's, uh. It's such a.

00:29:07 --> 00:29:10 It's almost a delightful film in. In some

00:29:10 --> 00:29:11 ways.

00:29:11 --> 00:29:13 Professor Fred Watson: Yeah. I thought it was a comedy, actually.

00:29:13 --> 00:29:14 Andrew Dunkley: Yeah, it bordered on that.

00:29:15 --> 00:29:15 Speaker D: That.

00:29:15 --> 00:29:15 Professor Fred Watson: Yeah.

00:29:15 --> 00:29:16 Speaker D: Yeah.

00:29:16 --> 00:29:19 Andrew Dunkley: And it sort of. It sort of had a little

00:29:19 --> 00:29:21 bit of the Muppet show in it at times,

00:29:22 --> 00:29:24 but. But it really was a great storey. I

00:29:24 --> 00:29:25 loved it.

00:29:25 --> 00:29:25 Professor Fred Watson: Yeah.

00:29:25 --> 00:29:27 Andrew Dunkley: Yeah, yeah. Thanks, Colin. Great to hear from

00:29:27 --> 00:29:29 you. Thanks to everyone who sent us

00:29:29 --> 00:29:31 questions. Don't forget you can do the same

00:29:31 --> 00:29:34 via our website, space nutspodcast.com space

00:29:34 --> 00:29:37 nuts IO and just click

00:29:37 --> 00:29:39 on the Ask Me Anything tab at the top. And

00:29:39 --> 00:29:40 don't forget to tell us who you are and where

00:29:40 --> 00:29:41 you're from. And have a look around while

00:29:41 --> 00:29:43 you're there. And don't forget to leave

00:29:43 --> 00:29:46 reviews wherever you listen or watch us. Um,

00:29:47 --> 00:29:49 they help. Don't know who they help. I don't

00:29:49 --> 00:29:50 know why they help, but apparently they help.

00:29:51 --> 00:29:53 Uh, unless they're not good reviews, then

00:29:53 --> 00:29:55 they don't help. See,

00:29:56 --> 00:29:59 that's, you know, that's harder to

00:29:59 --> 00:30:02 explain than time dilation. Uh, and thank,

00:30:02 --> 00:30:04 uh, you, Fred Watson, for your help today.

00:30:04 --> 00:30:05 Couldn't have done it without you.

00:30:05 --> 00:30:07 Professor Fred Watson: Uh, I don't think I could have done it

00:30:07 --> 00:30:09 without you either, Andrew. So there you go.

00:30:10 --> 00:30:12 Just as well we're here. You're welcome. And

00:30:12 --> 00:30:13 we'll talk again soon.

00:30:13 --> 00:30:15 Andrew Dunkley: We will. Professor Fred Watson Watson,

00:30:15 --> 00:30:16 astronomer at large, and thanks to Huw in the

00:30:16 --> 00:30:19 studio. Couldn't be here due to an issue with

00:30:19 --> 00:30:21 time dilation, but we're expecting him in the

00:30:21 --> 00:30:24 year 2154. And from me, Andrew

00:30:24 --> 00:30:26 Dunkley. Thanks for your company. We'll see

00:30:26 --> 00:30:28 you on the next episode of Space Nuts. Bye

00:30:28 --> 00:30:30 Bye. Oh, hang on. Bye Bye.

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